The SU(4) invariant interaction Lagrangians between baryons and pseudoscalar mesons as well as between baryons and vector mesons
can be written, respectively, as [1]}
\({\cal {L}}_{PBB}&=ig_{p}(a\phi ^{*\alpha \mu \nu }\gamma _{5}P_{\alpha }^{\beta }\phi _{\beta \mu \nu }+b\phi ^{*\alpha \mu \nu }\gamma _{5}P^{\beta }_{\alpha }\phi _{\beta \nu \mu }),\\ {\cal {L}}_{VBB}&=ig_{v}(c\phi ^{*\alpha \mu \nu }\gamma V_{\alpha }^{\beta }\phi _{\beta \mu \nu }+d\phi ^{*\alpha \mu \nu }\gamma V^{\beta }_{\alpha }\phi _{\beta \nu \mu }).\) 
